TWI470797B - Power transistor with protected channel - Google Patents

Power transistor with protected channel Download PDF

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TWI470797B
TWI470797B TW98101258A TW98101258A TWI470797B TW I470797 B TWI470797 B TW I470797B TW 98101258 A TW98101258 A TW 98101258A TW 98101258 A TW98101258 A TW 98101258A TW I470797 B TWI470797 B TW I470797B
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doped
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TW200941726A (en
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Budong You
Yang Lu
Marco A Zuniga
Hamza Yilmaz
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Volterra Semiconductor Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/26Bombardment with radiation
    • H01L21/263Bombardment with radiation with high-energy radiation
    • H01L21/265Bombardment with radiation with high-energy radiation producing ion implantation
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
    • H01L29/08Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions with semiconductor regions connected to an electrode carrying current to be rectified, amplified or switched and such electrode being part of a semiconductor device which comprises three or more electrodes
    • H01L29/0843Source or drain regions of field-effect devices
    • H01L29/0847Source or drain regions of field-effect devices of field-effect transistors with insulated gate
    • H01L29/0852Source or drain regions of field-effect devices of field-effect transistors with insulated gate of DMOS transistors
    • H01L29/0873Drain regions
    • H01L29/0878Impurity concentration or distribution
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/78Field effect transistors with field effect produced by an insulated gate
    • H01L29/7801DMOS transistors, i.e. MISFETs with a channel accommodating body or base region adjoining a drain drift region
    • H01L29/7816Lateral DMOS transistors, i.e. LDMOS transistors
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
    • H01L29/0684Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape, relative sizes or dispositions of the semiconductor regions or junctions between the regions
    • H01L29/0692Surface layout
    • H01L29/0696Surface layout of cellular field-effect devices, e.g. multicellular DMOS transistors or IGBTs
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/402Field plates
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/41Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
    • H01L29/423Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
    • H01L29/42312Gate electrodes for field effect devices
    • H01L29/42316Gate electrodes for field effect devices for field-effect transistors
    • H01L29/4232Gate electrodes for field effect devices for field-effect transistors with insulated gate
    • H01L29/42364Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the insulating layer, e.g. thickness or uniformity
    • H01L29/42368Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the insulating layer, e.g. thickness or uniformity the thickness being non-uniform

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  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Hardware Design (AREA)
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  • Insulated Gate Type Field-Effect Transistor (AREA)
  • Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)
  • Semiconductor Integrated Circuits (AREA)

Description

具保護通道的功率電晶體Power transistor with protective channel

本發明是關於半導體裝置。The present invention relates to a semiconductor device.

諸如DC-DC轉換器之電壓調節器乃用來提供電子系統穩定的電壓源。轉換電壓調節器(或簡稱「轉換調節器」)已知為有效的DC-DC轉換器。轉換調節器藉由將輸入DC電壓轉換成高頻電壓訊號而產生輸出電壓,並藉由過濾高頻輸入電壓訊號而產生輸出DC電壓。明確地說,轉換調節器包括交換器,用以交替耦合或消除輸入DC電壓源(如電池)與負載(如積體電路)間的耦合。一般包括誘導器和電容器的輸出濾波器係耦合於輸入電壓源與負載之間,以過濾交換器之輸出並因此提供輸出DC電壓。諸如脈衝寬度調變器或脈衝頻率調變器的控制器控制交換器,以維持實質不變的輸出DC電壓。A voltage regulator such as a DC-DC converter is used to provide a stable voltage source for the electronic system. A switching voltage regulator (or simply "switching regulator") is known as an efficient DC-DC converter. The switching regulator generates an output voltage by converting the input DC voltage into a high frequency voltage signal, and generates an output DC voltage by filtering the high frequency input voltage signal. In particular, the switching regulator includes a switch for alternately coupling or eliminating coupling between an input DC voltage source (such as a battery) and a load (such as an integrated circuit). An output filter, typically including an inducer and a capacitor, is coupled between the input voltage source and the load to filter the output of the converter and thereby provide an output DC voltage. A controller, such as a pulse width modulator or a pulse frequency modulator, controls the exchanger to maintain a substantially constant output DC voltage.

由於橫向擴散金氧半(LDMOS)電晶體在特徵導通電阻(Rdson )和汲極到源極崩潰電壓(BVd_s )方面的性能衡量結果,其可用於轉換調節器。導通電阻(Rdson )和裝置的長期可靠度又是另一個性能權衡。Due to the performance measurement of the laterally diffused gold-oxide half (LDMOS) transistor in terms of characteristic on-resistance (R dson ) and drain-to-source breakdown voltage (BV d_s ), it can be used for conversion regulators. The on-resistance (R dson ) and the long-term reliability of the device are another performance trade-off.

參照第1圖,傳統LDMOS電晶體300包括p型基材302,其內形成高壓n型井(HV n-井)304。HV n-井中有具n摻雜之n+區域312、p摻雜之p+區域314與p摻雜之p主體擴散區(p-主體)316的源極區310、具n摻雜之n+區域322與更輕摻雜之n型摻雜汲極(NDD)324的汲極區320、和具閘氧化層332與多晶矽層334的閘極330。Referring to Fig. 1, a conventional LDMOS transistor 300 includes a p-type substrate 302 in which a high voltage n-well (HV n-well) 304 is formed. The HV n-well has an n-doped n+ region 312, a p-doped p+ region 314 and a p-doped p-body diffusion region (p-body) 316 source region 310, n-doped n+ region 322 A drain region 320 with a lighter doped n-type doped drain (NDD) 324, and a gate 330 with a gate oxide layer 332 and a polysilicon layer 334.

在傳統LDMOS設計中,因形成空乏區來支援高汲極電壓電位,以致於在閘極330下方的NDD中且介於n+區域322與HV n-井304間的區域340會遭受到最大電場。由於區域340在導電時是位於電流路徑中,故已有相當程度的工程努力來縮減此高電阻區。然縮減高電阻區將進一步提高電場梯度及造成高碰撞游離率。故在傳統LDMOS設計中,區域340為關閉時發生裝置崩潰之處。In conventional LDMOS designs, the high drain voltage potential is supported by the formation of a depletion region such that the region 340 between the n+ region 322 and the HV n-well 304 in the NDD below the gate 330 experiences the maximum electric field. Since region 340 is in the current path when conducting, a considerable degree of engineering effort has been made to reduce this high resistance region. However, reducing the high resistance region will further increase the electric field gradient and cause high collision liberation rates. Therefore, in the conventional LDMOS design, the area 340 is where the device collapses when it is turned off.

當區域340發生崩潰時,此區域340會產生大量的電洞和電子。這些載子因具高能量而容易陷入裝置汲極側的閘氧化層內,導致裝置固有特性惡化及影響長期可靠度,例如場效應電晶體(FET)導通電阻降低。避免功率LDMOS裝置內部崩潰的一技術為與LDMOS裝置並聯設置崩潰電壓較小的第二裝置,以強行限制LDMOS裝置的汲極電壓。但此方式需要更複雜的系統、更多的組件數量和更高的成本。When region 340 collapses, this region 340 produces a large number of holes and electrons. These carriers are easily trapped in the gate oxide layer on the drain side of the device due to high energy, resulting in deterioration of the inherent characteristics of the device and affecting long-term reliability, such as a decrease in on-resistance of a field effect transistor (FET). One technique to avoid internal collapse of the power LDMOS device is to provide a second device with a small breakdown voltage in parallel with the LDMOS device to forcibly limit the gate voltage of the LDMOS device. But this approach requires more complex systems, more component counts, and higher costs.

在一態樣中,電晶體包括具p型主體之p型基材、形成於基材的n-井、形成於n-井的源極、形成於n-井且與源極相隔的汲極、供電流從汲極流向源極的通道區、閘極,用以控制位於源極與汲極間的通道區之通道形成、和崩潰區,位於通道區外的高壓n-井。源極包括p摻雜之p-主體、位於p-主體內的p摻雜之p+區域、和位於p-主體內的第一n摻雜之n+區域。汲極包括第二n摻雜之n+區域。崩潰區位於p-主體與基材之p型主體間。通道區具有內部崩潰電壓,崩潰區具有比內部崩潰電壓小的外來崩潰電壓。In one aspect, the transistor comprises a p-type substrate having a p-type body, an n-well formed on the substrate, a source formed in the n-well, a drain formed in the n-well and separated from the source a channel region and a gate for supplying current from the drain to the source, for controlling the channel formation and the collapse region of the channel region between the source and the drain, and the high voltage n-well outside the channel region. The source includes a p-doped p-body, a p-doped p+ region in the p-body, and a first n-doped n+ region in the p-body. The drain includes a second n-doped n+ region. The collapse zone is located between the p-body and the p-body of the substrate. The channel zone has an internal breakdown voltage, and the collapse zone has an external collapse voltage that is less than the internal breakdown voltage.

在另一態樣中,電晶體包括具p型主體之p型基材、形成於基材的n-井、形成於n-井的源極、形成於n-井且與源極相隔的汲極、供電流從汲極流向源極的通道區、閘極,用以控制位於源極與汲極間的通道區之通道形成、和崩潰區,位於通道區外的高壓n-井。源極包括p摻雜之p-主體、位於p-主體內的p摻雜之p+區域、和位於p-主體內的第一n摻雜之n+區域。汲極包括第二n摻雜之n+區域。崩潰區位於第二n摻雜之n+區域與基材之p型主體間。通道區具有內部崩潰電壓,崩潰區具有比內部崩潰電壓小的外來崩潰電壓。In another aspect, the transistor comprises a p-type substrate having a p-type body, an n-well formed on the substrate, a source formed in the n-well, a germanium formed in the n-well and separated from the source A channel, a gate for supplying current from the drain to the source, a channel for forming a channel region between the source and the drain, and a collapse region, and a high-voltage n-well outside the channel region. The source includes a p-doped p-body, a p-doped p+ region in the p-body, and a first n-doped n+ region in the p-body. The drain includes a second n-doped n+ region. The collapse zone is located between the second n-doped n+ region and the p-type body of the substrate. The channel zone has an internal breakdown voltage, and the collapse zone has an external collapse voltage that is less than the internal breakdown voltage.

任一上述態樣的實施例可包括一或多個下列特徵結構。基材上的場氧化物可圍繞n-井及延伸越過部分n-井。場氧化物可延伸越過部分p-主體。汲極可包括n摻雜區域,其圍繞第二n摻雜之n+區域且摻雜更輕。場氧化物可延伸越過部分n摻雜區域。第一n摻雜之n+區域可毗連p+區域。通道可沿著第一方向延伸,崩潰區沿著垂直第一方向的第二方向延伸。內部崩潰電壓比外來崩潰電壓大不超過約10%。內部崩潰電壓比外來崩潰電壓大約1-2伏特。汲極可為分散式汲極,具有複數個各自包括第二n摻雜之n+區域的汲極區,閘極可包括複數個閘線,用以控制介於源極與汲極區間的複數個空乏區。源極可為分散式源極,具有複數個各自包括p-主體、p+區域和第二n摻雜之n+區域的源極區,閘極可包括複數個閘線,用以控制介於源極區與汲極間的複數個空乏區。Embodiments of any of the above aspects may include one or more of the following features. The field oxide on the substrate can extend around the n-well and over a portion of the n-well. The field oxide can extend across a portion of the p-body. The drain may include an n-doped region that surrounds the second n-doped n+ region and is lighter doped. The field oxide can extend across a portion of the n-doped region. The first n-doped n+ region may be adjacent to the p+ region. The channel may extend along a first direction, the collapse zone extending in a second direction that is perpendicular to the first direction. The internal breakdown voltage is no more than about 10% greater than the external breakdown voltage. The internal breakdown voltage is approximately 1-2 volts than the external breakdown voltage. The drain may be a dispersed drain having a plurality of drain regions each including a second n-doped n+ region, and the gate may include a plurality of gate lines for controlling a plurality of sources between the source and the drain Vacant area. The source may be a decentralized source having a plurality of source regions each including a p-body, a p+ region, and a second n-doped n+ region, and the gate may include a plurality of gate lines for controlling the source A number of empty areas between the district and the bungee.

在又一態樣中,電晶體包括基材、形成於基材的井、汲極,包括植入井中的第一雜質區、源極,包括植入井中的第二雜質區且與第一雜質區相隔、供電流從汲極流向源極的通道、和閘極,用以控制介於源極與汲極間的空乏區。通道具有內部崩潰電壓,井、汲極和源極係配置成提供比內部崩潰電壓小的外來崩潰電壓,使崩潰得以發生在位於通道外且鄰接汲極或源極之井內的崩潰區。In still another aspect, the transistor includes a substrate, a well formed on the substrate, a drain, including a first impurity region, a source, and a second impurity region implanted in the well, and the first impurity The cells are separated by a channel for supplying current from the drain to the source, and a gate for controlling the depletion region between the source and the drain. The channel has an internal breakdown voltage, and the well, drain and source are configured to provide an external breakdown voltage that is less than the internal breakdown voltage, allowing the collapse to occur in a collapse zone located outside the channel and adjacent to the well of the drain or source.

實施例可包括一或多個下列特徵結構。汲極可為分散式汲極,具有複數個各自包括第一雜質區的汲極區,源極可為分散式源極,具有複數個各自包括第二雜質區的源極區,閘極可包括複數個閘線,用以控制介於源極區與汲極區間的複數個空乏區。複數個汲極和複數個源極可間隔排成多個行列。各行列可沿著第一方向延伸,高壓井中的崩潰區可沿著垂直第一方向的第二方向延伸。井中的崩潰區可設在各行列末端。汲極可為分散式汲極,具有複數個各自包括第一雜質區的汲極區,閘極可包括複數個閘線,用以控制介於源極與汲極區間的複數個空乏區。源極可為分散式源極,具有複數個各自包括第二雜質區的源極區,閘極可包括複數個閘線,用以控制介於源極區與汲極間的複數個空乏區。基材可為p型基材,井可為n型井。第一雜質區可為n摻雜之n+區域,第二雜質區為n摻雜之n+區域。源極可包括p摻雜之p+區域。源極可包括p摻雜之p-主體、第一雜質區和形成於p-主體內的p摻雜之p+區域。高壓井中的崩潰區可鄰接p-主體。汲極可包括n摻雜區域,其圍繞第二n摻雜之n+區域且摻雜更輕。基材上的場氧化物可圍繞n-井及延伸越過部分p-主體。基材上的場氧化物可圍繞高壓井及延伸越過部分高壓井。內部崩潰電壓比外來崩潰電壓大不超過約10%。內部崩潰電壓比外來崩潰電壓大約1-2伏特。閘極可包括第一導電區和電性隔離且獨立偏壓自第一導電區的第二導電區,第一導電區控制在源極的p-主體上之通道形成,第二導電區控制內部崩潰區的電位。Embodiments may include one or more of the following features. The drain may be a dispersed drain, having a plurality of drain regions each including a first impurity region, the source may be a distributed source, and having a plurality of source regions each including a second impurity region, the gate may include A plurality of gate lines are used to control a plurality of depletion zones between the source region and the drain region. A plurality of drains and a plurality of sources may be arranged in a plurality of rows and columns. Each row may extend along a first direction, and a collapse zone in the high pressure well may extend in a second direction that is perpendicular to the first direction. The collapse zone in the well can be located at the end of each rank. The drain may be a dispersed drain having a plurality of drain regions each including a first impurity region, and the gate may include a plurality of gate lines for controlling a plurality of depletion regions between the source and drain regions. The source may be a decentralized source having a plurality of source regions each including a second impurity region, and the gate may include a plurality of gate lines for controlling a plurality of depletion regions between the source region and the drain. The substrate can be a p-type substrate and the well can be an n-type well. The first impurity region may be an n-doped n+ region, and the second impurity region is an n-doped n+ region. The source can include a p-doped p+ region. The source may include a p-doped p-body, a first impurity region, and a p-doped p+ region formed in the p-body. The collapse zone in the high pressure well can be adjacent to the p-body. The drain may include an n-doped region that surrounds the second n-doped n+ region and is lighter doped. The field oxide on the substrate can extend around the n-well and over a portion of the p-body. The field oxide on the substrate can surround the high pressure well and extend across a portion of the high pressure well. The internal breakdown voltage is no more than about 10% greater than the external breakdown voltage. The internal breakdown voltage is approximately 1-2 volts than the external breakdown voltage. The gate may include a first conductive region and a second conductive region electrically isolated and independently biased from the first conductive region, the first conductive region controls channel formation on the p-body of the source, and the second conductive region controls the interior The potential of the collapse zone.

在再一態樣中,製造電晶體的方法包括選擇電晶體之源極和汲極中雜質區的尺寸和濃度、選擇n-井的n-井濃度,源極和汲極將形成於n-井中、選擇源極與汲極之雜質區間的距離、從尺寸、濃度、距離和n-井濃度,決定介於源極與汲極間之通道的內部崩潰電壓、以及選擇延伸越過源極的部分n-井的寬度,使部分之n-井的外來崩潰電壓比內部崩潰電壓小。In still another aspect, a method of fabricating a transistor includes selecting a size and concentration of an impurity region in a source and a drain of the transistor, selecting an n-well concentration of the n-well, and a source and a drain are formed in the n- In the well, select the distance between the source and the bucking impurity interval, the size, concentration, distance, and n-well concentration, determine the internal breakdown voltage of the channel between the source and the drain, and select the portion that extends beyond the source. The width of the n-well causes the external collapse voltage of some of the n-wells to be less than the internal collapse voltage.

實施例可包括一或多個下列特徵結構。基材可植入具選定尺寸和濃度的雜質區,及植入具選定n-井濃度和寬度的n-井。Embodiments may include one or more of the following features. The substrate can be implanted with an impurity region of selected size and concentration, and implanted with an n-well having a selected n-well concentration and width.

實施例可包括一或多個下列特徵結構。當崩潰發生時,碰撞游離產生的電子電洞對可遠離內部通道區。如此,FET導通電阻不需因突如其來的崩潰而降低。此法不會犧牲重要的矽區域。Embodiments may include one or more of the following features. When a crash occurs, the electron hole pair generated by the collision free can be far from the internal channel area. As such, the FET on-resistance does not need to be reduced due to sudden collapse. This method does not sacrifice important shackles.

一或多個實施例將配合所附圖式詳述於下。其他特徵、目的和優點在參閱說明書、圖式和後附申請專利範圍後,將變得更清楚易懂。One or more embodiments will be described in detail below in conjunction with the drawings. Other features, objects, and advantages will be apparent from the description and appended claims.

大體而言,本文是關於具有固有的自我保護能力的功率裝置。即,裝置設計成當崩潰發生時,碰撞游離產生的電子電洞對將遠離內部通道區(從汲極之n+區域到源極之n+/p+區域的直接電流路徑)。In general, this article is about power devices with inherent self-protection capabilities. That is, the device is designed such that when a crash occurs, the electron hole pair generated by the collision free will be away from the internal channel region (the direct current path from the n+ region of the drain to the n+/p+ region of the source).

大體而言,功率裝置是利用功率LDMOS並非一維應用裝置的事實。特別地,裝置可設計讓通道依循第一路徑(如沿著第一方向),且沿著第二方向發生崩潰(如沿著垂直的第二方向)。In general, power devices are the fact that power LDMOS is not a one-dimensional application. In particular, the device can be designed to have the channel follow a first path (eg, along a first direction) and collapse in a second direction (eg, along a second, vertical direction).

第2圖為LDMOS裝置100的平面圖。LDMOS電晶體100包括P型基材102,其內形成高壓n型井(HV n-井)104。HV n-井中有由閘極130隔開的源極區110和汲極區120。源極區110沿著閘極延伸的長度LS大於其垂直方向的寬度WS。同樣地,汲極區120沿著閘極延伸的長度LD大於其垂直方向的寬度WD。尺寸可從重摻雜區域的邊界算起。FIG. 2 is a plan view of the LDMOS device 100. The LDMOS transistor 100 includes a P-type substrate 102 in which a high voltage n-well (HV n-well) 104 is formed. The HV n-well has a source region 110 and a drain region 120 separated by a gate 130. The length LS of the source region 110 extending along the gate is greater than the width WS of its vertical direction. Similarly, the length LD of the drain region 120 extending along the gate is greater than the width WD of its vertical direction. The size can be calculated from the boundary of the heavily doped region.

源極區110和汲極區120可間隔排成多個行列,各行列被閘極130隔開。雖然只繪示一汲極區120,但圖案也可重複配置一個以上的汲極區120。同樣地,雖然只繪示二源極區110,但圖案也可重複配置二個以上的源極區110。又,單一源極區110的對側可配置二汲極區120。運作時,電流經由沿著閘極長度延伸的通道從汲極流向源極(如箭頭所指)。在一些實施例中,源極區的長度等於汲極區的長度。The source region 110 and the drain region 120 may be arranged in a plurality of rows and columns, and each row and column is separated by a gate 130. Although only one drain region 120 is shown, more than one of the drain regions 120 may be repeatedly arranged in the pattern. Similarly, although only the two source regions 110 are shown, the pattern may be repeatedly arranged with two or more source regions 110. Also, the opposite side of the single source region 110 can be configured with the second drain region 120. In operation, current flows from the drain to the source (as indicated by the arrow) via a channel extending along the length of the gate. In some embodiments, the length of the source region is equal to the length of the drain region.

第3A圖為與源極與汲極區寬度平行的截面圖。每一閘極130包括閘氧化層132和導電層134(如多晶矽層)於閘氧化層132上。在一些實施例中,閘氧化層包括靠近相鄰汲極區120的較厚區域、和靠近相鄰源極區110的較薄區域。各閘極連接共通控制電壓。Figure 3A is a cross-sectional view parallel to the width of the source and drain regions. Each gate 130 includes a gate oxide layer 132 and a conductive layer 134 (eg, a polysilicon layer) on the gate oxide layer 132. In some embodiments, the gate oxide layer includes a thicker region proximate to the adjacent drain region 120 and a thinner region proximate the adjacent source region 110. Each gate is connected to a common control voltage.

源極區110包括n摻雜之n+區域112、p摻雜之p+區域114和p摻雜之p-主體擴散區(p-主體)116。p-主體116圍繞n+區域112和p+區域114。n+區域112毗連p+區域114,且n+區域接近汲極區120。p-主體116的雜質濃度低於p+區域114。p-主體116和n+區域112(如於氧化物側壁前植入的斜線區)在閘氧化層132下方延伸,p-主體比n+區域延伸更遠。上金屬層的接觸墊136(參見第2圖)電性連接n+區域112和p+區域114。在一些實施例中,個別接觸墊同時接觸n+區域112和p+區域114。The source region 110 includes an n-doped n+ region 112, a p-doped p+ region 114, and a p-doped p-body diffusion region (p-body) 116. The p-body 116 surrounds the n+ region 112 and the p+ region 114. The n+ region 112 is adjacent to the p+ region 114, and the n+ region is adjacent to the drain region 120. The impurity concentration of the p-body 116 is lower than the p+ region 114. The p-body 116 and the n+ region 112 (as in the oblique region implanted in front of the oxide sidewall) extend below the gate oxide layer 132, and the p-body extends further than the n+ region. The contact pads 136 of the upper metal layer (see FIG. 2) are electrically connected to the n+ region 112 and the p+ region 114. In some embodiments, the individual contact pads simultaneously contact the n+ region 112 and the p+ region 114.

汲極區120包括n摻雜之n+區域122和更輕摻雜之n型摻雜汲極(NDD)124。NDD 124圍繞n+區域122。NDD在閘氧化層132下方延伸。上金屬層的接觸墊138(參見第2圖)電性連接n+區域122。The drain region 120 includes an n-doped n+ region 122 and a lighter doped n-type doped drain (NDD) 124. NDD 124 surrounds n+ region 122. NDD extends below the gate oxide layer 132. The contact pads 138 of the upper metal layer (see FIG. 2) are electrically connected to the n+ region 122.

HV n-井104的雜質濃度低於n+區域112、122和NDD 124。The impurity concentration of the HV n-well 104 is lower than the n+ regions 112, 122 and the NDD 124.

第3B圖為與源極長度平行的局部截面圖,例如與通過p+區域114的閘線平行。p-主體116在平行閘線的方向上比p+區域114延伸更遠。同樣地,HV n-井104在平行閘線的方向上比p-主體116延伸更遠。Figure 3B is a partial cross-sectional view parallel to the source length, for example parallel to the gate line passing through the p+ region 114. The p-body 116 extends further in the direction of the parallel gate line than the p+ region 114. Likewise, the HVn-well 104 extends further in the direction of the parallel gate line than the p-body 116.

主動區外的部分基材由場氧化物150覆蓋。p-主體116和HV n-井104在鄰近源極區110的場氧化物150下方延伸。場氧化物150可完全圍住HV n-井104。雖未繪示,但導電接觸點可設置直接接觸p型基材102,以於場氧化物150更遠處做為基材電極。A portion of the substrate outside the active region is covered by field oxide 150. The p-body 116 and the HV n-well 104 extend below the field oxide 150 adjacent the source region 110. Field oxide 150 can completely enclose HV n-well 104. Although not shown, the conductive contacts may be placed in direct contact with the p-type substrate 102 to serve as a substrate electrode further from the field oxide 150.

如圖所示,終止區140包括一部分的HV n-井104,其夾設在p-主體116與p型基材102之間。由於其位於源極區110的側邊(鄰接閘極130的邊緣對面),故此區域不當作通道。As shown, the termination region 140 includes a portion of the HV n-well 104 that is sandwiched between the p-body 116 and the p-type substrate 102. Since it is located on the side of the source region 110 (opposite the edge of the gate 130), this region is not considered a channel.

第3C圖為與汲極長度平行的局部截面圖,例如與通過n+區域122的閘線平行。NDD 124在平行閘線的方向上比n+區域122延伸更遠。同樣地,HV n-井104在平行閘線的方向上比NDD 124延伸更遠。Figure 3C is a partial cross-sectional view parallel to the length of the drain, for example parallel to the gate line passing through the n+ region 122. The NDD 124 extends further in the direction of the parallel gate line than the n+ region 122. Likewise, HVn-well 104 extends further away from NDD 124 in the direction of the parallel gate line.

如上所述,主動區外的部分基材由場氧化物150覆蓋。NDD 124和HV n-井104在鄰近汲極區120的場氧化物150下方延伸。As noted above, a portion of the substrate outside the active region is covered by field oxide 150. NDD 124 and HV n-well 104 extend below field oxide 150 adjacent to drain region 120.

如圖所示,終止區142包括一部分的HV n-井104,其夾設在NDD 124與p型基材102之間。由於其位於汲極區120的側邊(鄰接閘極130的邊緣對面),故此區域不當作通道。As shown, the termination region 142 includes a portion of the HV n-well 104 that is sandwiched between the NDD 124 and the p-type substrate 102. Since it is located on the side of the drain region 120 (opposite the edge of the gate 130), this region is not considered a channel.

裝置設計使得汲極到主體的外來崩潰電壓(如沿著3B-3B截面,從主體至基材之p型主體)略比裝置的內部崩潰電壓(如沿著3A-3A截面,通過通道)小。HV n-井104在p-主體116與p型基材102間的寬度(WHV)、和不同雜質區的濃度可選擇使終止區140的崩潰電壓小於通道的崩潰電壓。或者或此外,HV n-井104在NDD 124與p型基材102間的寬度(WHV)、和不同雜質區的濃度可選擇使終止區142的崩潰電壓小於通道的崩潰電壓,以致外來崩潰電壓(如沿著3C-3C截面,從NDD至基材之p型主體)略比裝置的內部崩潰電壓小。如此,當崩潰發生時,碰撞游離產生的電子電洞對將遠離內部通道區。故FET導通電阻不再因突如其來的崩潰而降低。The device is designed such that the external collapse voltage from the drain to the body (such as the p-body from the body to the substrate along the 3B-3B section) is slightly smaller than the internal breakdown voltage of the device (eg, along the 3A-3A section, through the channel) . The width (WHV) of the HV n-well 104 between the p-body 116 and the p-type substrate 102, and the concentration of the different impurity regions may be selected such that the breakdown voltage of the termination region 140 is less than the breakdown voltage of the channel. Alternatively or in addition, the width (WHV) of the HV n-well 104 between the NDD 124 and the p-type substrate 102, and the concentration of the different impurity regions may be selected such that the breakdown voltage of the termination region 142 is less than the breakdown voltage of the channel, such that the external breakdown voltage (eg, along the 3C-3C section, the p-type body from the NDD to the substrate) is slightly less than the internal breakdown voltage of the device. Thus, when a crash occurs, the pair of electron holes generated by the collision free will be far from the internal channel area. Therefore, the FET on-resistance is no longer reduced by sudden collapse.

此外,儘管第3B及3C圖繪示崩潰區140、142分別設在源極和汲極側當作陣列中最外面的源極或汲極區,其配置垂直閘線,然崩潰區亦可形成在源極或汲極側,其配置平行閘線134,但更遠離閘極和相關通道。In addition, although the 3B and 3C diagrams show that the collapse regions 140, 142 are respectively disposed on the source and drain sides as the outermost source or drain region in the array, and the vertical gate line is disposed, the collapse region can also be formed. On the source or drain side, it is configured with parallel gate lines 134, but further away from the gates and associated channels.

按照初級評估,外來路徑與內部路徑間的崩潰電壓差(ΔBV)可由崩潰事件之最大電流與外來崩潰路徑之串聯電阻的乘積判定。崩潰電壓差(ΔBV)可選擇小於外來崩潰電壓的10%。例如,若裝置之崩潰電壓為約30伏特,則植入區域的濃度和尺寸可選擇讓外來崩潰電壓為約30伏特,內部崩潰電壓為約32伏特。此新的裝置設計方法可達到裝置自我保護之目的,雖然稍微損失崩潰電壓值的ΔBV(1-2伏特),但不會犧牲重要的矽面積。According to the primary evaluation, the breakdown voltage difference (ΔBV) between the external path and the internal path can be determined by the product of the maximum current of the crash event and the series resistance of the external collapse path. The breakdown voltage difference (ΔBV) can be chosen to be less than 10% of the external breakdown voltage. For example, if the device has a breakdown voltage of about 30 volts, the concentration and size of the implanted region can be selected to have an external collapse voltage of about 30 volts and an internal breakdown voltage of about 32 volts. This new device design approach achieves the device's self-protection, although it slightly loses the ΔBV (1-2 volts) of the breakdown voltage value, but does not sacrifice important 矽 area.

達成內部與外來崩潰電壓差的方法實例將說明於下。利用熟知的功率LDMOS設計方式,可調整內部崩潰電壓成預定崩潰值。藉由改變置於二相同電位之p型區域間的高壓n-井寬度,可將此特殊裝置結構的外來崩潰電壓調整成預定崩潰電壓減去ΔBV的值。An example of a method for achieving an internal and external breakdown voltage difference will be described below. With the well-known power LDMOS design, the internal breakdown voltage can be adjusted to a predetermined crash value. The external collapse voltage of this particular device structure can be adjusted to a predetermined breakdown voltage minus the value of ΔBV by varying the high voltage n-well width placed between the p-type regions of the same potential.

第4圖繪示另一實施例,其中各閘極130包括二電性隔離之閘極130a、130b,其偏壓成不同電位。每一閘極130a、130b包括閘氧化層132和導電層134(如多晶矽層)於閘氧化層132上。閘極130a、130b可平行延伸。靠近源極區110的閘極130a設在突出n+區域112的部分p-主體116上,而可通過p-主體116控制通道形成。靠近汲極的閘極130b設在伸出n+區域122的部分NDD 124和其餘通道部分(除了HV n-井104外,其可未經摻雜)上,而可控制內部崩潰區的電壓電位。故選擇閘極130a、130b上的電壓可挑選崩潰電壓值和崩潰位置。FIG. 4 illustrates another embodiment in which each gate 130 includes two electrically isolated gates 130a, 130b that are biased at different potentials. Each of the gates 130a, 130b includes a gate oxide layer 132 and a conductive layer 134 (eg, a polysilicon layer) on the gate oxide layer 132. The gates 130a, 130b may extend in parallel. A gate 130a adjacent to the source region 110 is disposed on a portion of the p-body 116 that protrudes from the n+ region 112, and channel formation can be controlled by the p-body 116. A gate 130b adjacent to the drain is provided on a portion of the NDD 124 extending beyond the n+ region 122 and the remaining channel portion (which may be undoped except for the HVn-well 104) to control the voltage potential of the internal collapse region. Therefore, the voltage on the gates 130a, 130b can be selected to select the breakdown voltage value and the collapse location.

本發明已以一些實施例揭露如上。然應理解在不脫離本發明之精神和範圍內,其當可作各種之更動與潤飾。例如,雖然在此是敘述p型主體和p型基材,但p型基材當可以其他可用之p型植入代替。因此,其他實施例亦落在後附申請專利範圍所界定之範圍內。The present invention has been disclosed above in some embodiments. It is to be understood that various changes and modifications may be made without departing from the spirit and scope of the invention. For example, although a p-type body and a p-type substrate are described herein, the p-type substrate can be replaced by other p-type implants that are available. Therefore, other embodiments are also within the scope defined by the scope of the appended claims.

100...電晶體100. . . Transistor

102...基材102. . . Substrate

104...井104. . . well

110...源極區110. . . Source area

112、114、122...區域112, 114, 122. . . region

116...主體116. . . main body

120...汲極區120. . . Bungee area

124...汲極124. . . Bungee

130、130a、130b...閘極130, 130a, 130b. . . Gate

132...閘氧化層132. . . Gate oxide layer

134...導電層134. . . Conductive layer

136、138...接觸墊136, 138. . . Contact pad

140、142...終止區/崩潰區140, 142. . . Termination area/crash area

150...場氧化物150. . . Field oxide

300...電晶體300. . . Transistor

302...基材302. . . Substrate

304...井304. . . well

310...源極區310. . . Source area

312、314、322、340...區域312, 314, 322, 340. . . region

320...汲極區320. . . Bungee area

324...汲極324. . . Bungee

330...閘極330. . . Gate

332...閘氧化層332. . . Gate oxide layer

334...多晶矽層334. . . Polycrystalline layer

第1圖為傳統LDMOS電晶體的截面圖。Figure 1 is a cross-sectional view of a conventional LDMOS transistor.

第2圖為LDMOS電晶體之一實施例的平面圖。Figure 2 is a plan view of one embodiment of an LDMOS transistor.

第3A、3B及3C圖為第2圖LDMOS電晶體的截面圖。3A, 3B, and 3C are cross-sectional views of the LDMOS transistor of Fig. 2.

第4圖為LDMOS電晶體之另一實施例的截面圖。Figure 4 is a cross-sectional view of another embodiment of an LDMOS transistor.

各圖中相同的元件符號代表相似的元件。The same element symbols in the various figures represent similar elements.

102...基材102. . . Substrate

104...井104. . . well

110...源極區110. . . Source area

112、114、122...區域112, 114, 122. . . region

116...主體116. . . main body

120...汲極區120. . . Bungee area

124...汲極124. . . Bungee

130...閘極130. . . Gate

134...導電層134. . . Conductive layer

136、138...接觸墊136, 138. . . Contact pad

Claims (55)

一種電晶體,包含:一p型基材,具有一p型主體;一n-井,形成於該基材中;一源極,形成於該n-井中且包括:一p摻雜之p-主體;一p摻雜之p+區域,位於該p-主體內;以及一第一n摻雜之n+區域,位於該p-主體內;一汲極,形成於該n-井中且與該源極相隔開,該汲極包括一第二n摻雜之n+區域;一通道區,供電流從該汲極流向該源極,該通道區具有一內部崩潰電壓(intrinsic breakdown voltage);一閘極,用以控制位於該源極與該汲極之間的該通道區中之通道形成;以及一崩潰區,位於該通道區外且位於該p-主體與該基材之該p型主體之間的該n-井中,其中該崩潰區與該通道區的摻雜(doping)與尺寸(dimensions)之設計,會使得該崩潰區的一外來(extrinsic)崩潰電壓比該內部崩潰電壓小。 A transistor comprising: a p-type substrate having a p-type body; an n-well formed in the substrate; a source formed in the n-well and comprising: a p-doped p- a body; a p-doped p+ region located within the p-body; and a first n-doped n+ region located within the p-body; a drain formed in the n-well and with the source Separated, the drain includes a second n-doped n+ region; a channel region for current to flow from the drain to the source, the channel region having an intrinsic breakdown voltage; a gate, Forming a channel for controlling the channel region between the source and the drain; and a collapse region located outside the channel region and between the p-body and the p-body of the substrate In the n-well, the doping and dimensions of the collapse zone and the channel zone are designed such that an extrinsic breakdown voltage of the collapse zone is less than the internal breakdown voltage. 如申請專利範圍第1項所述之電晶體,更包含一場氧化物,位於該基材上且圍繞該n-井及延伸越過一部分的該n-井。 The transistor of claim 1, further comprising a field oxide on the substrate and surrounding the n-well and extending over a portion of the n-well. 如申請專利範圍第2項所述之電晶體,其中該場氧化物延伸越過一部分的該p-主體。 The transistor of claim 2, wherein the field oxide extends over a portion of the p-body. 如申請專利範圍第1項所述之電晶體,其中該內部崩潰電壓比該外來崩潰電壓大不超過約10%。 The transistor of claim 1, wherein the internal breakdown voltage is no more than about 10% greater than the external breakdown voltage. 如申請專利範圍第1項所述之電晶體,其中該內部崩潰電壓比該外來崩潰電壓大約1-2伏特。 The transistor of claim 1, wherein the internal breakdown voltage is about 1-2 volts greater than the external breakdown voltage. 如申請專利範圍第1項所述之電晶體,其中該汲極包含一n摻雜區域,該n摻雜區域圍繞該第二n摻雜之n+區域且比該第二n摻雜之n+區域更少量地摻雜。 The transistor of claim 1, wherein the drain includes an n-doped region surrounding the second n-doped n+ region and than the second n-doped n+ region Doped in a smaller amount. 如申請專利範圍第1項所述之電晶體,其中該第一n摻雜之n+區域毗連(abut)該p+區域。 The transistor of claim 1, wherein the first n-doped n+ region abuts the p+ region. 如申請專利範圍第1項所述之電晶體,其中該通道區沿著一第一方向而延伸,該崩潰區沿著垂直於該第一方向的一第二方向而延伸。 The transistor of claim 1, wherein the channel region extends along a first direction, the collapse region extending along a second direction perpendicular to the first direction. 如申請專利範圍第1項所述之電晶體,其中該汲極為一分散式汲極,具有複數個各自包括該第二n摻雜之n+區域的汲極區,且該閘極包括複數個閘線,用以控制位於該源極與該些汲極區之間的複數個空乏區。 The transistor of claim 1, wherein the germanium is a decentralized drain having a plurality of drain regions each including the second n-doped n+ region, and the gate includes a plurality of gates a line for controlling a plurality of depletion regions between the source and the drain regions. 如申請專利範圍第1項所述之電晶體,其中該源極為一分散式源極,具有複數個各自包括該p-主體、該p+區域和該第一n摻雜之n+區域的源極區,且該閘極包括複數個閘線,用以控制位於該些源極區與該汲極之間的複數個空乏區。 The transistor of claim 1, wherein the source is a decentralized source having a plurality of source regions each including the p-body, the p+ region, and the first n-doped n+ region And the gate includes a plurality of gate lines for controlling a plurality of depletion regions between the source regions and the drain. 一種電晶體,包含:一p型基材,具一p型主體;一n-井,形成於該基材中;一源極,形成於該n-井中且包括:一p摻雜之p-主體;一p摻雜之p+區域,位於該p-主體內;以及一第一n摻雜之n+區域,位於該p-主體內;一汲極,形成於該n-井中且與該源極相隔開,該汲極包括一第二n摻雜之n+區域;一通道區,供電流從該汲極流向該源極,該通道區具有一內部崩潰電壓;一閘極,用以控制位於該源極與該汲極之間的該通道區中之通道形成;以及一崩潰區,位於該通道區外且位於該第二n摻雜之n+區域與該基材之該p型主體之間的該n-井中,其中該崩潰區與該通道區的摻雜與尺寸之設計,會使得該崩潰區的一外來崩潰電壓比該內部崩潰電壓小。 A transistor comprising: a p-type substrate having a p-type body; an n-well formed in the substrate; a source formed in the n-well and comprising: a p-doped p- a body; a p-doped p+ region located within the p-body; and a first n-doped n+ region located within the p-body; a drain formed in the n-well and with the source Separated, the drain includes a second n-doped n+ region; a channel region for current flow from the drain to the source, the channel region having an internal breakdown voltage; and a gate for controlling the location Forming a channel in the channel region between the source and the drain; and a collapse region located outside the channel region and between the second n-doped n+ region and the p-type body of the substrate In the n-well, the doping and size design of the collapse zone and the channel zone may cause an external collapse voltage of the collapse zone to be smaller than the internal breakdown voltage. 如申請專利範圍第11項所述之電晶體,其中該內部崩潰電壓比該外來崩潰電壓大不超過約10%。 The transistor of claim 11, wherein the internal breakdown voltage is no more than about 10% greater than the external breakdown voltage. 如申請專利範圍第11項所述之電晶體,其中該內部崩潰電壓比該外來崩潰電壓大約1-2伏特。 The transistor of claim 11, wherein the internal breakdown voltage is about 1-2 volts greater than the extraneous breakdown voltage. 如申請專利範圍第11項所述之電晶體,更包含一場氧化物,位於該基材上且圍繞該n-井及延伸越過一部分的該n-井。 The transistor of claim 11, further comprising a field oxide on the substrate and surrounding the n-well and extending over a portion of the n-well. 如申請專利範圍第14項所述之電晶體,其中該汲極包含一n摻雜區域,該n摻雜區域圍繞該第二n摻雜之n+區域且比該第二n摻雜之n+區域更少量地摻雜。 The transistor of claim 14, wherein the drain includes an n-doped region surrounding the second n-doped n+ region and than the second n-doped n+ region Doped in a smaller amount. 如申請專利範圍第15項所述之電晶體,其中該場氧化物延伸越過一部分的該n摻雜區域。 The transistor of claim 15 wherein the field oxide extends over a portion of the n-doped region. 如申請專利範圍第11項所述之電晶體,其中該第一n摻雜之n+區域毗連該p+區域。 The transistor of claim 11, wherein the first n-doped n+ region is adjacent to the p+ region. 如申請專利範圍第11項所述之電晶體,其中該通道區沿著一第一方向而延伸,該崩潰區沿著垂直於該第一方向的一第二方向而延伸。 The transistor of claim 11, wherein the channel region extends along a first direction, the collapse region extending along a second direction perpendicular to the first direction. 如申請專利範圍第11項所述之電晶體,其中該汲極為一分散式汲極,具有複數個各自包括該第二n摻雜之n+區域的汲極區,且該閘極包括複數個閘線,用以控制位於該源極與該些汲極區之間的複數個空乏區。 The transistor of claim 11, wherein the germanium is a decentralized drain having a plurality of drain regions each including the second n-doped n+ region, and the gate includes a plurality of gates a line for controlling a plurality of depletion regions between the source and the drain regions. 如申請專利範圍第11項所述之電晶體,其中該源極為一分散式源極,具有複數個各自包括該p-主體、該p+區域和該第一n摻雜之n+區域的源極區,且該閘極包括複數個閘線,用以控制位於該些源極區與該汲極之間的複數個空乏區。 The transistor of claim 11, wherein the source is a decentralized source having a plurality of source regions each including the p-body, the p+ region, and the first n-doped n+ region And the gate includes a plurality of gate lines for controlling a plurality of depletion regions between the source regions and the drain. 一種電晶體,包含:一基材;一井,形成於該基材中;一汲極,包括植入於該井中的一第一雜質區;一源極,包括植入於該井中且與該第一雜質區相隔開的一第二雜質區;一通道,供電流從該汲極流向該源極,該通道具有一內部崩潰電壓;以及一閘極,用以控制位於該源極與該汲極之間的一空乏區;一崩潰區,該崩潰區係在該井中,該井中的該崩潰區係位於該通道外且鄰接於該汲極或該源極,其中該井、該汲極和該源極的摻雜與尺寸被配置成,會使得該崩潰區 的一外來崩潰電壓比該內部崩潰電壓小,以便崩潰的發生係在位於該通道外且鄰接於該汲極或該源極的該井中的該崩潰區中。 A transistor comprising: a substrate; a well formed in the substrate; a drain comprising a first impurity region implanted in the well; a source comprising implanted in the well and a second impurity region separated by a first impurity region; a channel for supplying current from the drain to the source, the channel having an internal breakdown voltage; and a gate for controlling the source and the gate a depletion zone between the poles; in the collapse zone, the collapse zone is in the well, the collapse zone in the well being located outside the channel and adjacent to the drain or the source, wherein the well, the bungee and The source is doped and sized to cause the collapse zone An extraneous breakdown voltage is less than the internal collapse voltage so that the collapse occurs in the collapse zone located outside the channel and adjacent to the drain or the source. 如申請專利範圍第21項所述之電晶體,其中該汲極為一分散式汲極,具有複數個各自包括該第一雜質區的汲極區,該源極為一分散式源極,具有複數個各自包括該第二雜質區的源極區,且該閘極包括複數個閘線,用以控制位於該些源極區與該些汲極區之間的複數個空乏區。 The transistor of claim 21, wherein the germanium is a decentralized drain having a plurality of drain regions each including the first impurity region, the source being a decentralized source having a plurality of Each of the source regions of the second impurity region is included, and the gate includes a plurality of gate lines for controlling a plurality of depletion regions between the source regions and the drain regions. 如申請專利範圍第22項所述之電晶體,其中該些複數個汲極區和該些複數個源極區以交錯列(alternating rows)的方式來排列。 The transistor of claim 22, wherein the plurality of drain regions and the plurality of source regions are arranged in an alternating row. 如申請專利範圍第23項所述之電晶體,其中該些列沿著一第一方向而延伸,該崩潰區沿著垂直於該第一方向的一第二方向而延伸。 The transistor of claim 23, wherein the columns extend along a first direction, the collapse region extending along a second direction perpendicular to the first direction. 如申請專利範圍第23項所述之電晶體,其中該井中的該崩潰區係在該些列的一端(end)。 The transistor of claim 23, wherein the collapse zone in the well is at an end of the columns. 如申請專利範圍第21項所述之電晶體,其中該汲極為一分散式汲極,具有複數個各自包括該第一雜質區的 汲極區,且該閘極包括複數個閘線,用以控制位於該源極與該些汲極區之間的複數個空乏區。 The transistor of claim 21, wherein the crucible is a decentralized drain having a plurality of respective first impurity regions. a drain region, and the gate includes a plurality of gate lines for controlling a plurality of depletion regions between the source and the drain regions. 如申請專利範圍第21項所述之電晶體,其中該源極為一分散式源極,具有複數個各自包括該第二雜質區的源極區,且該閘極包括複數個閘線,用以控制位於該些源極區與該汲極之間的複數個空乏區。 The transistor of claim 21, wherein the source is a decentralized source having a plurality of source regions each including the second impurity region, and the gate includes a plurality of gate lines for A plurality of depletion regions between the source regions and the drain are controlled. 如申請專利範圍第21項所述之電晶體,其中該基材為一p型基材,該井為一n型井。 The transistor of claim 21, wherein the substrate is a p-type substrate, and the well is an n-type well. 如申請專利範圍第28項所述之電晶體,其中該第一雜質區為一第一n摻雜之n+區域,且該第二雜質區為一第二n摻雜之n+區域。 The transistor of claim 28, wherein the first impurity region is a first n-doped n+ region, and the second impurity region is a second n-doped n+ region. 如申請專利範圍第29項所述之電晶體,其中該源極包含一p摻雜之p+區域。 The transistor of claim 29, wherein the source comprises a p-doped p+ region. 如申請專利範圍第30項所述之電晶體,其中該源極包含一p摻雜之p-主體,該第二雜質區和該p摻雜之p+區域形成於該p-主體內。 The transistor of claim 30, wherein the source comprises a p-doped p-body, and the second impurity region and the p-doped p+ region are formed in the p-body. 如申請專利範圍第31項所述之電晶體,其中該崩潰區鄰接於該p-主體。 The transistor of claim 31, wherein the collapse zone is adjacent to the p-body. 如申請專利範圍第31項所述之電晶體,其中該汲極包含一n摻雜區域,該n摻雜區域圍繞該第一n摻雜之n+區域且比該第一n摻雜之n+區域更少量地摻雜。 The transistor of claim 31, wherein the drain includes an n-doped region surrounding the first n-doped n+ region and than the first n-doped n+ region Doped in a smaller amount. 如申請專利範圍第31項所述之電晶體,更包含一場氧化物,位於該基材上且圍繞該n型井及延伸越過一部分的該p-主體。 The transistor of claim 31, further comprising a field oxide, located on the substrate and surrounding the n-well and extending over a portion of the p-body. 如申請專利範圍第21項所述之電晶體,更包含一場氧化物,位於該基材上且圍繞該井及延伸越過一部分的該井。 The transistor of claim 21, further comprising a field oxide, located on the substrate and surrounding the well and extending over a portion of the well. 如申請專利範圍第21項所述之電晶體,其中該內部崩潰電壓比該外來崩潰電壓大不超過約10%。 The transistor of claim 21, wherein the internal breakdown voltage is no more than about 10% greater than the external breakdown voltage. 如申請專利範圍第21項所述之電晶體,其中該內部崩潰電壓比該外來崩潰電壓大約1-2伏特。 The transistor of claim 21, wherein the internal breakdown voltage is about 1-2 volts greater than the extraneous breakdown voltage. 如申請專利範圍第21項所述之電晶體,其中該閘極包含一第一導電區和電性隔離且獨立偏壓自該第一導電區的一第二導電區,該第一導電區控制在該源極中的一p-主體上之通道形成,該第二導電區控制在內部崩潰的區域中的一電位。 The transistor of claim 21, wherein the gate comprises a first conductive region and a second conductive region electrically isolated from the first conductive region, the first conductive region is controlled A channel is formed on a p-body in the source, the second conductive region controlling a potential in an area where the interior collapses. 一種製造一電晶體的方法,包含以下步驟:選擇用於該電晶體之一源極和一汲極中的雜質區的尺寸和濃度(concentrations);選擇一n-井的一n-井濃度,該源極和該汲極將形成於該n-井中;選擇該源極與該汲極之該些雜質區之間的一距離;從該些尺寸、該些濃度、該距離和該n-井濃度,來決定位於該源極與該汲極之間之一通道區的一內部崩潰電壓;以及選擇有延伸越過該源極的一部分的該n-井的一寬度,以提供會使得具有比該內部崩潰電壓小的一外來崩潰電壓的該部分的該n-井。 A method of fabricating a transistor comprising the steps of: selecting a size and concentration of an impurity region for a source and a drain of the transistor; selecting an n-well concentration of an n-well, The source and the drain will be formed in the n-well; a distance between the source and the impurity regions of the drain is selected; from the dimensions, the concentrations, the distance, and the n-well a concentration to determine an internal collapse voltage of a channel region between the source and the drain; and selecting a width of the n-well extending across a portion of the source to provide a The internal breakdown voltage is small for an alien crash voltage of that portion of the n-well. 如申請專利範圍第39項所述之方法,更包含以下步驟:(i)將該基材植入具有該些選擇的尺寸和濃度的該些雜質區、以及(ii)將該基材植入具有該選擇的n-井濃度和寬度的該n-井。 The method of claim 39, further comprising the steps of: (i) implanting the substrate into the impurity regions having the selected size and concentration, and (ii) implanting the substrate The n-well having the selected n-well concentration and width. 如申請專利範圍第40項所述之方法,其中該基材具有一p型主體,且將該基材植入該些雜質區的步驟包含以下步驟:(i)在一源極區中植入一p摻雜之p-主體、(ii)在該p-主體內植入一p摻雜之p+區域、(iii)在該p-主體內植入一第一n摻雜之n+區域、及(iv)在一汲極區中植 入一第二n摻雜之n+區域。 The method of claim 40, wherein the substrate has a p-type body, and the step of implanting the substrate into the impurity regions comprises the steps of: (i) implanting in a source region a p-doped p-body, (ii) implanting a p-doped p+ region in the p-body, (iii) implanting a first n-doped n+ region in the p-body, and (iv) planting in a bungee area Into a second n-doped n+ region. 如申請專利範圍第41項所述之方法,其中該部分的該n-井係位於該通道區外且位於該p-主體與該基材之該p型主體之間。 The method of claim 41, wherein the n-well is located outside the channel region and between the p-body and the p-body of the substrate. 如申請專利範圍第41項所述之方法,其中該部分的該n-井係位於該通道區外且位於該第二n摻雜之n+區域與該基材之該p型主體之間。 The method of claim 41, wherein the n-well is located outside the channel region and between the second n-doped n+ region and the p-body of the substrate. 如申請專利範圍第41項所述之方法,包含以下步驟:形成一閘極,以控制位於該源極與該汲極之間的該通道區中之通道形成。 The method of claim 41, comprising the step of forming a gate to control channel formation in the channel region between the source and the drain. 如申請專利範圍第41項所述之方法,包含以下步驟:沉積(deposit)一場氧化物於該基材上且圍繞該n-井及延伸越過一部分的該n-井。 The method of claim 41, comprising the step of depositing a layer of oxide on the substrate and surrounding the n-well and extending over a portion of the n-well. 如申請專利範圍第45項所述之方法,其中該場氧化物係被沉積以延伸越過一部分的該p-主體。 The method of claim 45, wherein the field oxide is deposited to extend over a portion of the p-body. 如申請專利範圍第44項所述之方法,其中將該基材植入該些雜質區的步驟包含以下步驟:(i)形成該汲極如同具有複數個各自包括第一雜質區的汲極區的一分散式 汲極、及(ii)形成該源極如同具有複數個各自包括第二雜質區的源極區的一分散式源極,及其中形成該閘極之步驟包含以下步驟:形成複數個閘線,以控制位於該些源極區與該些汲極區之間的複數個空乏區。 The method of claim 44, wherein the step of implanting the substrate into the impurity regions comprises the steps of: (i) forming the drain as if there are a plurality of drain regions each including a first impurity region Decentralized a drain, and (ii) forming the source as a decentralized source having a plurality of source regions each including a second impurity region, and the step of forming the gate includes the steps of: forming a plurality of gate lines, To control a plurality of depletion regions located between the source regions and the drain regions. 如申請專利範圍第47項所述之方法,包含以下步驟:形成以交錯列的方式來排列的該些複數個汲極區和該些複數個源極區。 The method of claim 47, comprising the steps of: forming the plurality of bungee regions arranged in a staggered column and the plurality of source regions. 如申請專利範圍第48項所述之方法,其中該些列沿著一第一方向而延伸,且該部分的該n-井沿著垂直於該第一方向的一第二方向而延伸。 The method of claim 48, wherein the columns extend along a first direction and the n-well of the portion extends along a second direction perpendicular to the first direction. 如申請專利範圍第48項所述之方法,其中該部分的該n-井係在該些列的一端。 The method of claim 48, wherein the n-well of the portion is at one end of the columns. 如申請專利範圍第41項所述之方法,其中將該基材植入該些雜質區的步驟包含以下步驟:在該汲極中植入一n摻雜區域,該n摻雜區域圍繞該第二n摻雜之n+區域且比該第二n摻雜之n+區域更少量地摻雜。 The method of claim 41, wherein the step of implanting the substrate into the impurity regions comprises the step of implanting an n-doped region in the drain, the n-doped region surrounding the first The n-doped n+ region is doped a little less than the second n-doped n+ region. 如申請專利範圍第51項所述之方法,其中該第一n摻雜之n+區域係被沉積以毗連該p+區域。 The method of claim 51, wherein the first n-doped n+ region is deposited to adjoin the p+ region. 如申請專利範圍第41項所述之方法,包含以下步驟:植入該些雜質區,會使得該通道區沿著一第一方向而延伸,且該部分沿著垂直於該第一方向的一第二方向而延伸。 The method of claim 41, comprising the step of implanting the impurity regions such that the channel region extends along a first direction and the portion is along a direction perpendicular to the first direction Extending in the second direction. 如申請專利範圍第39項所述之方法,其中該些尺寸、該些濃度、該距離和該寬度的選擇,會使得該內部崩潰電壓比該外來崩潰電壓大不超過約10%。 The method of claim 39, wherein the selection of the dimensions, the concentrations, the distances, and the widths causes the internal collapse voltage to be no more than about 10% greater than the extraneous breakdown voltage. 如申請專利範圍第39項所述之方法,其中該些尺寸、該些濃度、該距離和該寬度的選擇,會使得該內部崩潰電壓比該外來崩潰電壓大約1-2伏特。The method of claim 39, wherein the selection of the dimensions, the concentrations, the distances, and the width causes the internal breakdown voltage to be about 1-2 volts greater than the extraneous breakdown voltage.
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